{
  "annotation_id": "07d5bcc0-ea0a-4d1c-a76c-e04873aed608",
  "date_created": "2026-03-02T18:00:15.256000Z",
  "date_modified": "2026-03-02T18:00:15.256000Z",
  "file_hash": "350cc0f65e0da43b66138f240000724ea10c438a2877fd7e9595f5d6cb63111d",
  "private": false,
  "record": {
    "abstract": "Pion-meson-exchange nucleon-nucleon potentials are derived for two nucleons\nin the intermediate states. The mesons we include are (i) pseudoscalar mesons:\n$\\pi, \\eta, \\eta\u0027$; (ii) vector mesons: $\\rho, \\omega, \\phi$; (iii) scalar\nmesons: $a_{0}(980), \\varepsilon(760), f_{0}(975)$; and (iv) the $J=0$\ncontribution from the Pomeron. Strong dynamical pair suppression is assumed,\nand at the nucleon-nucleon-meson vertices Gaussian form factors are\nincorporated into the relativistic two-body framework using a dispersion\nrepresentation for the pion- and meson-exchange amplitudes. The Fourier\ntransformations are performed using factorization techniques for the energy\ndenominators. The potentials are first calculated in the adiabatic\napproximation to all planar and crossed three-dimensional momentum-space\n$\\pi$-meson diagrams. Next, we calculate the $1/M$ corrections.",
    "arxiv_id": "nucl-th/9509029",
    "authors": [
      "Th. A. Rijken",
      "V. G. J. Stoks"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.54.2851",
    "journal_ref": "Phys.Rev.C54:2851-2868,1996",
    "title": "Soft two-meson-exchange nucleon-nucleon potentials. I. Planar and   crossed-box diagrams",
    "url": "https://arxiv.org/abs/nucl-th/9509029"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "def51d9f-c186-4860-a2a0-1f84439c412e",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}